FRET Efficiency Calculator
Calculate FRET efficiency, donor-acceptor distance, and Förster radius for FRET experiments.
Why the Sixth Power Matters So Much
FRET efficiency depends on the inverse sixth power of donor–acceptor separation, which makes it extraordinarily distance-sensitive.
| r relative to R0 | Efficiency |
|---|---|
| 0.5 R0 | 98.5% |
| R0 | 50% by definition |
| 1.5 R0 | 8% |
| 2 R0 | 1.5% |
Doubling the distance reduces efficiency 64-fold. This is why FRET works as a molecular ruler over roughly 0.5 to 1.5 times R0 — typically 2 to 10 nm — and gives essentially no information outside that window.
That range happens to match the dimensions of protein-protein interactions and conformational changes, which is why the technique is so widely used despite its narrow window.
What Determines R0
| Factor | Effect |
|---|---|
| Spectral overlap | Donor emission must overlap acceptor absorption |
| Donor quantum yield | Higher yield raises R0 |
| Orientation factor κ² | Ranges 0 to 4; assumed 2/3 |
| Refractive index | Minor |
The orientation factor is the main source of uncertainty. It is conventionally assumed to be 2/3, which holds only if both dipoles rotate freely during the excited-state lifetime. Rigidly held fluorophores can give κ² anywhere from 0 to 4, and since R0 depends on its sixth root, the distance error can be substantial.
Measuring Efficiency
Donor quenching is the simplest approach but requires a matched sample lacking acceptor. Acceptor photobleaching is more robust: bleach the acceptor and the donor signal recovers in proportion to the FRET that was occurring, providing an internal control within the same cell.
Fluorescence lifetime imaging is more rigorous still, since donor lifetime shortens with FRET and is independent of concentration and excitation intensity — the two largest sources of artefact in intensity-based measurements.
Worked Examples
Common Mistakes
Efficiency saturates near 100% below and approaches zero above. Distances outside that range cannot be resolved.
That value assumes free rotation. Constrained dipoles can give values from 0 to 4, introducing substantial distance error.
It requires a matched donor-only sample. Acceptor photobleaching provides an internal control within the same specimen.
Donor emission detected in the acceptor channel inflates apparent FRET. Correction using single-labelled controls is essential.